TY - JOUR
T1 - High-pressure single-crystal X-ray diffraction study of katoite hydrogarnet
T2 - Evidence for a phase transition from Ia3d → I4̄3d symmetry at 5 GPa
AU - Lager, George A.
AU - Downs, Robert T.
AU - Origlieri, Marcus
AU - Garoutte, Rebecca
PY - 2002
Y1 - 2002
N2 - The crystal structure of katoite hydrogarnet has been refined at 0.0001, 2.15, 4.21, 5.09, 6.00, 7.09, and 7.78 GPa from single-crystal X-ray diffraction data using a 4:1 methanol: ethanol mixture as pressure medium in a Merrill-Bassett diamond-anvil cell. Below ~5 GPa, the katoite structure has la3d symmetry and compresses by bond shortening rather than bond bending, in agreement with recent quantum mechanical calculations. An unconstrained third-order Birch-Murnaghan fit to the unit-cell volumes and pressures for la3d symmetry gave the following equation of state parameters: Vo = 1987.6(1) Å3, Ko = 58(1) GPa and K' = 4.0(7). Above this pressure, the structure undergoes a phase transition to space group I43d, a non-centric subgroup of la3d. In the I43d structure. there are two non-equivalent (O4H4) groups. Both the Ca and Al atoms are displaced along a relative to their positions in la3d. It is proposed that compression of the short H-H distance between (O4H4) groups destabilizes the structure and may initiate the observed phase transition. Corroboration of this model will require accurate information on the hydrogen atom positions at pressures above 5 GPa.
AB - The crystal structure of katoite hydrogarnet has been refined at 0.0001, 2.15, 4.21, 5.09, 6.00, 7.09, and 7.78 GPa from single-crystal X-ray diffraction data using a 4:1 methanol: ethanol mixture as pressure medium in a Merrill-Bassett diamond-anvil cell. Below ~5 GPa, the katoite structure has la3d symmetry and compresses by bond shortening rather than bond bending, in agreement with recent quantum mechanical calculations. An unconstrained third-order Birch-Murnaghan fit to the unit-cell volumes and pressures for la3d symmetry gave the following equation of state parameters: Vo = 1987.6(1) Å3, Ko = 58(1) GPa and K' = 4.0(7). Above this pressure, the structure undergoes a phase transition to space group I43d, a non-centric subgroup of la3d. In the I43d structure. there are two non-equivalent (O4H4) groups. Both the Ca and Al atoms are displaced along a relative to their positions in la3d. It is proposed that compression of the short H-H distance between (O4H4) groups destabilizes the structure and may initiate the observed phase transition. Corroboration of this model will require accurate information on the hydrogen atom positions at pressures above 5 GPa.
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U2 - 10.2138/am-2002-5-606
DO - 10.2138/am-2002-5-606
M3 - Article
AN - SCOPUS:0036355857
SN - 0003-004X
VL - 87
SP - 642
EP - 647
JO - American Mineralogist
JF - American Mineralogist
IS - 5-6
ER -